“…The problem of sound waves corresponds to the propagation of forced waves, and consists in assuming a given real angular frequency ω and solving the dispersion relation (24) for a complex wavenumber κ as function of the oscillation frequency, that is κ = κ(ω). Then, the phase velocity and the attenuation coefficient of the waves can be computed from the roots of the dispersion relation, following a rather standard procedure (see, for example, [7,10,11,12,13,14,15]).…”